Violation of charge conjugation-parity ($\rm CP$) symmetry plays a major rule in the dominance of matter in our universe. A kind of $\rm CP$ violation results from the asymmetry of the life time measured in $M^0$ and $\bar M^0$, here $M$ is a heavy meson, decays to final states which is referred in the literature as $A_{ \Gamma}^f$. In this paper, we give an estimation of the upper bound on $|A_{ \Gamma}^f|$ for the Cabibbo Favored $D^0 \rightarrow K^- \pi^+$ decay process in different models. We show that in the standard model, $|A_{ \Gamma}^f| \lesssim\mathcal{ O} (10^{ -10})$. Recently a bound on $A_{ \Gamma}^f$ has been obtained: $(A^f_{ \Gamma})^{ Exp.}= (1.6 \pm 1)\times 10^{ -4}$. This result motivates further studies on $A_{ \Gamma}^f$ in beyond standard model physics. In the framework of two Higgs doublet model with generic Yukawa structure, we show that $|A_\Gamma^{ f}|\lesssim \mathcal{ O} (10^{ -7})$ which is several orders of magnitude smaller than the current experimental value. Finally, in the framework of left-right symmetric models in which the mixing between the left and the right gauge bosons is allowed and the left-right symmetry is not manifest at unification scale, we find that $A_{ \Gamma}^f$ can be as large as $|A_{ \Gamma}^f|\lesssim\mathcal{ O} (10^{ -5})$ which is one order of magnitude smaller than the experimentally measured value by LHCb collaborators.
Categories: hep-ph